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| Query : 2009MNRAS.394.2065K |
2009MNRAS.394.2065K - Mon. Not. R. Astron. Soc., 394, 2065-2079 (2009/April-3)
NLTE models of line-driven stellar winds - III. Influence of X-ray radiation on wind structure of O stars.
KRTICKA J. and KUBAT J.
Abstract (from CDS):
We show that the influence of shock X-ray emission on wind mass-loss rate is relatively small. Wind terminal velocity may be slightly influenced by the presence of strong X-ray sources, especially for stars cooler than Teff≲ 35000K.
We discuss the origin of the LX/L ∼ 10–7 relation. For stars with thick wind this relation can be explained assuming that the cooling time depends on wind density. Stars with optically thin winds exhibiting the `weak wind problem' display enhanced X-ray emission which may be connected with large shock cooling length. We propose that this effect can explain the `weak wind problem'.
Inclusion of X-rays leads to a better agreement of the model ionization structure with observations. However, we do not find any significant influence of X-rays on Pv ionization fraction implying that the presence of X-rays cannot explain the Pv problem.
We study the implications of modified ionization equilibrium due to shock emission on the line transfer in the X-ray region. We conclude that the X-ray line profiles of helium-like ions may be affected by the line absorption within the cool wind.
Abstract Copyright: © 2009 The Authors. Journal compilation © 2009 RAS
Journal keyword(s): hydrodynamics - stars: early-type - stars: mass-loss - stars: winds, outflows - X-rays: stars
Simbad objects: 16
| Number of rows : 16 |
| N | Identifier | Otype |
ICRS (J2000) RA |
ICRS (J2000) DEC |
Mag U | Mag B | Mag V | Mag R | Mag I | Sp type |
#ref
1850 - 2026 |
#notes |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| 1 | * ksi Per | ** | 03 58 57.9024302099 | +35 47 27.709515737 | 3.190 | 4.080 | 4.060 | 3.88 | 3.89 | O7.5III(n)((f)) | 850 | 0 |
| 2 | * alf Cam | s*b | 04 54 03.0113886719 | +66 20 33.633625509 | 3.47 | 4.34 | 4.29 | 4.18 | 4.18 | O9Ia | 675 | 1 |
| 3 | V* AE Aur | Or* | 05 16 18.1493304816 | +34 18 44.344404000 | 5.48 | 6.18 | 5.96 | O9.5V | 597 | 1 | ||
| 4 | NAME LMC | G | 05 23 34.6 | -69 45 22 | 0.4 | ~ | 19090 | 0 | ||||
| 5 | * lam Ori A | Em* | 05 35 08.2760807112 | +09 56 02.991326316 | 2.17 | 3.48 | 3.47 | O8III((f)) | 527 | 0 | ||
| 6 | * mu. Col | V* | 05 45 59.8950238944 | -32 18 23.162261796 | 3.84 | 4.90 | 5.18 | 5.30 | 5.57 | O9.5V | 523 | 0 |
| 7 | HD 42088 | * | 06 09 39.5728368936 | +20 29 15.450599580 | 6.73 | 7.58 | 7.57 | 8.45 | O6V((f))z | 257 | 0 | |
| 8 | HD 46202 | bC* | 06 32 10.4706981304 | +04 57 59.764912343 | 7.60 | 8.332 | 8.269 | 7.98 | 7.86 | O9.2V | 300 | 0 |
| 9 | HD 54662 | SB* | 07 09 20.2493151288 | -10 20 47.635088964 | 5.35 | 6.24 | 6.21 | 7.23 | O6.5Vz(n)+O7.5Vz | 354 | 0 | |
| 10 | HD 93204 | * | 10 44 32.3390794992 | -59 44 31.020804780 | 7.63 | 8.52 | 8.42 | 8.20 | 7.92 | O5.5V((f)) | 200 | 0 |
| 11 | * bet Cru | bC* | 12 47 43.26877 | -59 41 19.5792 | 0.03 | 1.02 | 1.25 | 1.38 | 1.64 | B1IV | 360 | 1 |
| 12 | * zet Oph | Be* | 16 37 09.5400587698 | -10 34 01.509742704 | 1.73 | 2.58 | 2.56 | 2.46 | 2.50 | O9.2IVnn | 1908 | 0 |
| 13 | * 63 Oph | * | 17 54 54.0432011904 | -24 53 13.544140416 | 5.35 | 6.24 | 6.20 | 7.33 | O8II((f)) | 185 | 0 | |
| 14 | * 68 Cyg | SB* | 21 18 27.1862219256 | +43 56 45.399147864 | 4.05 | 4.99 | 5.00 | O7.5IIIn((f)) | 383 | 0 | ||
| 15 | * 19 Cep | * | 22 05 08.7897533088 | +62 16 47.332569936 | 4.36 | 5.19 | 5.11 | 4.95 | 4.92 | O9Ib | 397 | 0 |
| 16 | * lam Cep | s*b | 22 11 30.5765111040 | +59 24 52.154264880 | 4.55 | 5.29 | 5.05 | 4.77 | 4.62 | O6.5I(n)fp | 705 | 1 |
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